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Some representative refractive indices
Materialn at λ=589.3 nm
Vacuum1 (exactly)
Helium1.000036
Air at STP1.0002926
carbon dioxide1.00045
water ice1.31
liquid water (20°C)1.333
cryolite1.338
ethanol1.36
glycerine1.4729
rock salt1.516
glass (typical)1.5 to 1.9
Crown glass1.52
salt (NaCl) 1.544
polycarbonate1.59
bromine1.661
cubic zirconia2.15 to 2.18
diamond2.419
moissanite (silicon carbide)2.65 to 2.69
cinnabar (mercury sulfide)3.02
gallium phosphide3.5
gallium arsenide3.927
silicon4.01

Many materials have a well-characterized refractive index, but these indices depend strongly upon the wavelength of light. Therefore, any numeric value for the index is meaningless unless the associated wavelength is specified.

There are also weaker dependencies on temperature, pressure/stress, et cetera, as well on precise material compositions (presence of dopants et cetera); for many materials and typical conditions, however, these variations are at the percent level or less. Thus, it is especially important to cite the source for an index measurement if precision is required.

In general, an index of refraction is a complex number with both a real and imaginary part, where the latter indicates the strength of absorption loss at a particular wavelength—thus, the imaginary part is sometimes called the extinction coefficient k. Such losses become particularly significant, for example, in metals at short (e.g. visible) wavelengths, and must be included in any description of the refractive index.

See also


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טבלת מקדמי השבירה | Lijst van brekingsindices

 

This article is licensed under the GNU Free Documentation License. It uses material from the "List of indices of refraction".

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